Experimental evidence of bulk chemistry constraint on SiO2 solubility in clinopyroxene at high-pressure conditions

Lithos ◽  
2015 ◽  
Vol 226 ◽  
pp. 4-16 ◽  
Author(s):  
Toshisuke Kawasaki ◽  
Yasuhito Osanai
2017 ◽  
Vol 7 (1) ◽  
Author(s):  
Z. Wojnarowska ◽  
M. Rams-Baron ◽  
J. Knapik-Kowalczuk ◽  
A. Połatyńska ◽  
M. Pochylski ◽  
...  

As a result of a variety of experiments it was suggested in 1928 that engine “knock” “appears to be due to inequality in the condition of the charge (in the engine cylinder) set up, particularly in regions of high pressure and temperature as in the neighbourhood of hot exhaust valves. This inequality provides regions of high energy containing molecules in high energy states where reaction can spread more quickly.” This view was a little vague, and was arrived at from indirect experimental evidence. It was with a view to obtaining more precise evidence that knock was occasioned in the flame as the result of processes of slow combustion occurring in the gaseous charge prior to its arrival that the present work was undertaken. Callendar and those working with him had simultaneously arrived at the conclusion that “knock” was occasioned in much the same manner, but they adopted the more definite view that peroxides of the hydrocarbons were formed and stored in the gas, and then suddenly detonated, so igniting a whole region of the gas simultaneously. This view had also been advanced by Moureu and Dufraisse.


2019 ◽  
Vol 528 ◽  
pp. 115832 ◽  
Author(s):  
Sarah Incel ◽  
Alexandre Schubnel ◽  
Jörg Renner ◽  
Timm John ◽  
Loïc Labrousse ◽  
...  

1974 ◽  
Vol 39 (307) ◽  
pp. 768-787 ◽  
Author(s):  
R. N. Thompson

SummaryMicroprobe analyses of Ca-rich pyroxenes crystallized in the melting ranges of a magnesian alkali basalt, a transitional basalt, an olivine tholeiite, a tholeiitic andesite, and an augite leucitite at pressures between 8 and 45 kb show complex variation. Ca-poor pyroxene precipitated only from the alkali basalt at pressures between 14 and 18 kb. Pyroxene falling near the Di-Hed join in the pyroxene quadilateral formed at all pressures and temperatures from the leucitite, whereas ‘Ca-rich’ pyroxene crystallizing from the other four compositions was Ca-poor augite to sub-calcic augite. The liquidus Ca-rich pyroxenes all show rising Al and Na and falling Ti with increasing pressure and temperature. Other elements show complex behaviour; all but the leucitite pyroxenes tend to make temporary excursions of solid solution towards Ca-poor pyroxene at intermediate pressures, returning to more Ca-rich compositions at high pressures. At sub-liquidus temperatures Na and Ti consistently rise with falling T at constant P and also with rising P at constant T in these pyroxenes. The behaviour of the other elements in these circumstances depends on the nature of the coexisting phases.Fe/Mg distribution between Ca-rich pyroxene and liquid, in the form has a constant value of 0.29 for three separate bulk compositions at widely differing temperatures and pressures. Distribution coefficients for Mg and Fe between pyroxenes and coexisting garnets at high pressures are very similar to those found in garnet pyroxenite xenoliths from Oahu, Hawaii. Systematic shifts in the apparent stoichiometry (all Fe taken as Fe2+) of the augite leucitite pyroxenes are thought to indicate that they have considerable Fe3+ contents at low pressure, decreasing as P rises. If so, they show a strong negative correlation between Na and Fe3+, which negates the customary practice of forming acmite before jadeite component when recalculating the analyses of high-pressure pyroxenes.The sets of pyroxenes crystallized from each composition show consistent trends when plotted on such diagrams as jadeite vs Ca-Tschermak's ‘molecule’, which have often been used in attempts to discriminate natural pyroxenes formed in differing P-T environments. However, these new data show clearly that the bulk chemistry of the magma has a predominating influence on the composition of the pyroxenes crystallizing from it. Unless it is certain that a suite of natural pyroxenes have all precipitated from the same magma, it is probably pointless to attempt to deduce the relative P-T conditions of their formation from their major element chemistry.


2004 ◽  
Vol 93 (10) ◽  
Author(s):  
Florent Occelli ◽  
Daniel L. Farber ◽  
James Badro ◽  
Chantel M. Aracne ◽  
David M. Teter ◽  
...  

1979 ◽  
Vol 193 (1) ◽  
pp. 359-367
Author(s):  
I. G. Crow ◽  
J. C. Greene ◽  
J. D. Tyldesley ◽  
M. A. Walker

The behaviour of acid, neutral and alkali feedwater contaminants, which may be present in the AGR's (Advanced Gas Cooled Reactor) boilers has been examined in a test loop operating at 14.5 MPa. It has been found that deposition occurred at all contamination levels tested (1.5 μg kg-1 to 3200 μg kg-1 sodium) and could be attributed to two processes: a chemisorption reaction occurring between the steam and the dry tube walls, and at higher contamination levels, a gross deposition mechanism in the region of final dryout which experimental evidence suggests was associated with liquid film dryout.


2005 ◽  
Vol 2005 (1) ◽  
pp. 26-30 ◽  
Author(s):  
Arne Allwardt ◽  
Norbert Stoll ◽  
Christian Wendler ◽  
Kerstin Thurow

Catalytic high-pressure reactions play an important role in classic bulk chemistry. The optimization of common reactions, the search for new and more effective catalysts, and the increasing use of catalytic pressure reactions in the field of drug development call for high-parallel reaction systems. A crucial task of current developments, apart from the parameters of pressure, temperature, and number of reaction chambers, is, in this respect, the systems' integration into complex laboratory automation environments.


2021 ◽  
Author(s):  
Jorge Hirsch ◽  
Frank Marsiglio

Abstract The Meissner effect, magnetic field expulsion, is a hallmark of superconductivity. Associated with it, superconductors exclude applied magnetic fields. Recently Minkov et al. presented experimental results reportedly showing ``definitive evidence of the Meissner effect'' in sulfur hydride and lanthanum hydride under high pressure [1]. Instead, we show here that the evidence presented in that paper does not support the case for superconductivity in these materials. Together with experimental evidence discussed in earlier papers, we argue that this clearly indicates that hydrides under pressure are not high temperature superconductors.


1984 ◽  
Vol 62 (6) ◽  
pp. 569-576 ◽  
Author(s):  
R. D. Verma

Predissociation in the B3Πg, ν = 12 level of N2 is reexamined from a study of the 12–8 band of the [Formula: see text] transition in absorption as well as in emission under different conditions. New intensity perturbations are discovered at N′ = 27 and 28 for the R22 and R33 branches respectively and at about N′ = 29 for the Q11, Q22, and Q33 branches. These intensity perturbations, as well as the one already known at about N = 33, are suppressed in emission by increasing the pressure of N2. A new break-off point at N′ ≥ 42 is observed at high pressure. The analysis of these results confirms the existence of a [Formula: see text] state with a shallow potential well. The experimental molecular parameters of the [Formula: see text]state are in good agreement with the theoretical values.


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